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2011 QCD and High Energy Interactions - Rencontres de Moriond ...

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Figure 1: Helix string parametrizations. Left: original proposal (Eq.1). Right: modified helix scenario (Eq.2).<br />

The lines in the string area diagram connect points with i<strong>de</strong>ntical helix phase.<br />

A modified version of the helix string scenario has been proposed in 3 , with helix phase<br />

difference proportional to the amount of energy stored in the <strong>QCD</strong> string ( in the string rest<br />

frame )<br />

∆Φ = S κ ∆l (2)<br />

where S is a parameter, κ is string energy <strong>de</strong>nsity, <strong>and</strong> ∆l is distance (along the string) separating<br />

points with helix phase difference ∆Φ.<br />

The difference between mo<strong>de</strong>ls is illustrated by Fig. 1. In the original helix string scenario,<br />

the helix winding becomes faster towards string endpoints, while the modified scenario <strong>de</strong>fines<br />

a regular, static helix structure.<br />

3 Experimental signature<br />

The modified helix string fragmentation scenario (Eq.2) predicts a number of features which<br />

can be observed experimentally. The size of transverse momentum pT of a direct hadron is<br />

correlated with its energy E ( in the rest frame of the string) via relation<br />

| pT | = 2 r|sin(0.5 S E)| (3)<br />

where r st<strong>and</strong>s for radius of the helix structure. The correlations are shown in Fig. 2 (left) for a<br />

toy case of simple hadronic system without hard gluon kinks. Fig. 2 (right) shows the difference<br />

between the st<strong>and</strong>ard pT mo<strong>de</strong>lling ( via tunneling ) <strong>and</strong> the helix driven pT mo<strong>de</strong>lling in the<br />

inclusive pT spectrum. Direct observation of E−pT correlations is difficult due to the smearing by<br />

parton shower, but the qualitative difference in the shape of the inclusive spectrum is preserved.<br />

Interestingly enough, such type of discrepancy is readily observed in hadronic data 4,5 .<br />

The parameters of the helix string mo<strong>de</strong>l have been adjusted using LEP data with help of<br />

Rivet/Professor tools 6 . A simultaneous tuning of 6 parameters (including helix radius r, pitch<br />

S, Lund parameters (a,b), parton shower cut-off <strong>and</strong> effective coupling constant Λ<strong>QCD</strong>) has been<br />

performed for two parton shower algorithms (Pythia pT or<strong>de</strong>red parton shower 7 <strong>and</strong> Ariadne<br />

parton shower 8 ) interfaced to private implementation of the helix string fragmentation algorithm

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